The amyloid hypothesis causatively relates the fibrillar deposits of amyloid β peptide (Aβ) to Alzheimer's disease (AD). More recent data, however, identify the soluble oligomers as the major cytotoxic entities. Pyroglutamylated Aβ (pE-Aβ) is present in AD brains and exerts augmented neurotoxicity, which is believed to result from its higher β-sheet propensity and faster fibrillization. While this concept is based on a set of experimental results, others have reported similar β-sheet contents in unmodified and pyroglutamylated Aβ, and slower aggregation of pE-Aβ as compared to unmodified Aβ, leaving the issue unresolved. Here, we assess the structural differences between Aβ and pE-Aβ peptides that may underlie their distinct cytotoxicities. Transmission electron microscopy identifies a larger number of prefibrillar aggregates of pE-Aβ at early stages of aggregation and suggests that pE-Aβ affects the fibrillogenesis even at low molar fractions. Circular dichroism and FTIR data indicate that while the unmodified Aβ readily forms β-sheet fibrils in aqueous media, pE-Aβ displays increased α-helical and decreased β-sheet propensity. Moreover, isotope-edited FTIR spectroscopy shows that pE-Aβ reverses β-sheet formation and hence fibrillogenesis of the unmodified Aβ peptide via a prion-like mechanism. These data provide a novel structural mechanism for pE-Aβ hypertoxicity; pE-Aβ undergoes faster formation of prefibrillar aggregates due to its increased hydrophobicity, thus shifting the initial stages of fibrillogenesis toward smaller, hypertoxic oligomers of partial α-helical structure.
The amyloid hypothesis causatively relates the fibrillar deposits of amyloid β peptide (Aβ) to Alzheimer's disease (AD). More recent data, however, identify the soluble oligomers as the major cytotoxic entities. Pyroglutamylated Aβ (pE-Aβ) is present in AD brains and exerts augmented neurotoxicity, which is believed to result from its higher β-sheet propensity and faster fibrillization. While this concept is based on a set of experimental results, others have reported similar β-sheet contents in unmodified and pyroglutamylated Aβ, and slower aggregation of pE-Aβ as compared to unmodified Aβ, leaving the issue unresolved. Here, we assess the structural differences between Aβ and pE-Aβ peptides that may underlie their distinct cytotoxicities. Transmission electron microscopy identifies a larger number of prefibrillar aggregates of pE-Aβ at early stages of aggregation and suggests that pE-Aβ affects the fibrillogenesis even at low molar fractions. Circular dichroism and FTIR data indicate that while the unmodified Aβ readily forms β-sheet fibrils in aqueous media, pE-Aβ displays increased α-helical and decreased β-sheet propensity. Moreover, isotope-edited FTIR spectroscopy shows that pE-Aβ reverses β-sheet formation and hence fibrillogenesis of the unmodified Aβ peptide via a prion-like mechanism. These data provide a novel structural mechanism for pE-Aβ hypertoxicity; pE-Aβ undergoes faster formation of prefibrillar aggregates due to its increased hydrophobicity, thus shifting the initial stages of fibrillogenesis toward smaller, hypertoxic oligomers of partial α-helical structure.
Alzheimer’s disease
(AD) is a neurodegenerative disorder
characterized by neuronal and synaptic loss leading to cognitive and
memory impairment. Extracellular fibrillar deposits (plaques) of amyloid-β
(Aβ) peptide have been found in the AD brain and thought to
be causatively related to the disease.[1−3] However, currently accumulated
evidence identifies the soluble oligomers of Aβ as the main
neurotoxic entities.[4−8]Aβ is a proteolytic product of the amyloid precursor
protein
and can contain varying numbers of amino acid residues, with the 40-
and 42-residue peptides (Aβ1–40 and Aβ1–42) being the prevalent forms. Circular dichroism
(CD) and NMR data indicate that in organic solvents such as hexafluoroisopropanol
(HFIP) Aβ1–42 adopts a partially α-helical
structure and in the presence of >80% H2O acquires a
β-sheet
structure.[9] In aqueous media, Aβ
forms fibrils composed of β-sheets where the strand axis is
approximately perpendicular and the H-bonding is parallel to the long
fibrillar axis, known as a cross β-sheet structure.[10,11] Antiparallel β-sheets were proposed to constitute the core
structural motif of fibrils formed by Aβ1–42 or its fragments.[12,13] However, solid state NMR studies
on Aβ1–42 and shorter peptides identified
in-register parallel β-sheet structures,[14−16] consistent
with models derived from spin-label EPR,[17] solution NMR,[18] and Fourier transform
infrared (FTIR) studies.[19,20] Apparent inconsistencies
might originate from different stages of peptideaggregation in different
samples, as Aβ1–42 oligomers and fibrils were
shown by FTIR to adopt antiparallel and parallel β-sheet structures,
respectively.[21]Significant amounts
of N-terminally truncated and pyroglutamylated
(at Glu3 or Glu11) Aβ peptide (pE-Aβ) have been identified
in AD brains and shown to aggregate at increased rates[22−26] and to be more cytotoxic than unmodified Aβ.[27,28] Even at low fractions, pE-Aβ coaggregates with Aβ by
a seeding mechanism and forms structurally distinct and highly toxic
oligomers.[27] Dot-blot experiments using
conformation-sensitive antibodies showed that the highly toxic oligomers
containing 5% or less pE-Aβ were structurally different from
the mildly toxic unmodified Aβ aggregates of similar size.[27] While these studies imply a structural mechanism
for augmented toxicity of pE-Aβ, the underlying structural differences
between Aβ and pE-Aβ remain uncharacterized. Solution
NMR showed that AβpE3–40 in trifuoroethanol/water
(2:3) has a reduced α-helical propensity compared to Aβ1–40,[29] consistent with a
significantly higher β-sheet content and faster fibrillogenesis
of pE-Aβ.[23,25] Conversely, CD studies identified
similar content of β-sheet in both unmodified Aβ and pE-Aβ
peptides,[30] and fibrillogenesis of AβpE3-42 was reported to be significantly slower compared
to Aβ1–42.[31] These
conflicting data on fibrillogenesis of unmodified Aβ and pE-Aβ
are evidently related to the inherent polymorphism and sensitivity
of the Aβ peptides to the experimental conditions and procedures.[32,33] Since the content of pE-Aβ in AD brains varies in a wide range
and affects the structure and the toxicity of the amyloid aggregates,[27,34,35] individual structures of unmodified
Aβ and pE-Aβ separately and in combination, as well as
the mutual structural effects, should be determined to shed light
on the molecular mechanism underlying the altered fibrillogenesis
of pE-Aβ.Here, we have employed transmission electron
microscopy (TEM),
CD, and FTIR spectroscopy to analyze structural transitions in Aβ1–42 and AβpE3-42 peptides during
fibrillogenesis. Isotope-edited FTIR was used to examine structural
changes in both peptides combined in one sample, which allowed identification
of the profound prion-like conformational effect of pE-Aβ on
the unmodified Aβ. Specifically, pE-Aβ not only exhibited
an increased α-helical and reduced β-sheet propensity
but also was able to retard β-sheet formation by Aβ and
to reverse β-sheets to α-helical structure at initial
stages of fibrillogenesis. These findings suggest that the augmented
cytotoxicity of pE-Aβ may result from its preference to form
hypertoxic aggregates of partial α-helical structure as opposed
to mildly toxic β-sheet fibrils.
Materials
and Methods
Materials
The Aβ1–42 and uniformly 13C-labeled Aβ1–42 peptides were purchased
from rPeptide (Bogart, GA, USA) and were >97% pure. AβpE3-42 was from Innovagen (Lund, Sweden) and was 98%
pure. The peptides
were analyzed by MALDI-TOF mass-spectrometry at the ICBR Proteomics
Core Facility of the University of Florida (Gainesville, FL, USA),
and the amino acid compositions of all three peptides were confirmed.
Salts, buffers, HFIP, and other chemicals were from Fisher Scientific
(Hanover Park, IL, USA) or Sigma-Aldrich (St. Louis, MO, USA).
Experimental
Procedures
In all experiments, the lyophilized
peptides were initially dissolved in HFIP at 200 μM concentration
to disperse any preformed aggregates. In TEM experiments, appropriate
amounts of the peptides were dried in a glass vial by desiccation
for 15 min, followed by incubation in an aqueous buffer of 50 mM NaCl
+ 50 mM Na,K-phosphate (pH 7.2) at 37 °C with constant stirring
for 24 h. TEM samples were prepared following the procedures described
by Nilsson,[36] i.e., by deposition of 5
μL of peptide suspension on the grid, incubation for 5 min,
and rinsing with 4 μL of distilled/deionized water, followed
by staining for 30 s with 2 μL of 3% uranyl acetate, washing
twice with 5 μL of distilled/deionized water, and air-drying.
Grids for the negative control experiments were prepared by identical
procedures using 5 μL of blank buffer instead of the peptide
suspension. Images were acquired on a JEOL TEM-1011 operated at 80
kV using thin (<3 nm) holey carbon grids (Ted Pella, Inc., Redding,
CA, USA).In CD experiments, the HFIP solutions of peptides
were dried by desiccation in a 4 mm × 4 mm quartz cuvette and
spectra were collected between 180 and 330 nm to determine the structure
of the dry peptides. Subsequently, an aqueous buffer of 50 mM NaCl
+ 50 mM Na,K-phosphate (pH 7.2) was added to a 50 μM final concentration
of the peptides and spectra were acquired consecutively for 24 h to
identify secondary structural changes upon fibrillogenesis at 37 °C
with constant stirring, using a J-810 spectropolarimeter (Jasco, Tokyo,
Japan). To improve the signal-to-noise ratio, the spectra were smoothed
using a 13-point Savitzky-Golay linear least-squares algorithm embedded
in the Igor Pro 5.03 software.FTIR experiments were conducted
to determine the structure of the
peptides in desiccated form, nominally hydrated by atmospheric humidity,
and in the presence of excess aqueous buffer. Desired amounts of the
peptides were dissolved in HFIP at 200 μM concentration, and
40 μL of the solution was placed on a CaF2 FTIR window
and dried in a desiccator for 15 min. FTIR spectra of the peptide
samples were collected while the peptide was allowed to absorb humidity
from the atmosphere as monitored by the increase in the H2O stretching band intensity around 3270 cm–1. Then,
80 μL of aqueous buffer (10 mM Na,K-phosphate in D2O, pD 7.2, corresponding to the pH-meter reading of 6.8) was added
to the peptide and the sample was sealed by a second window using
a 50 μm-thick Teflon spacer, followed by measurements of spectra
of the peptide in aqueous medium. The spectra were measured by coadding
500 scans on a Vector-22 FTIR spectrometer (Bruker Optics, Billerica,
MA, USA) equipped with a liquid nitrogen-cooled Hg–Cd–Te
detector, at 2 cm–1 nominal resolution at 25 °C,
as described earlier.[37] Reference transmission
spectra were collected using either a single CaF2 window
or the buffer sealed between two windows and were used to calculate
the absorbance spectra. H2O vapor spectra were measured
separately and subtracted from the sample spectra when necessary.
The spectra were smoothed as described above, and baseline correction
was applied.
Results
Based on
earlier findings that AβpE3-42 forms aggregates
that are structurally different from the aggregates
of Aβ1–42 and exert prion-like toxicity on
cultured neurons,[27] we hypothesized that
AβpE3-42 modulates the structure of the unmodified
peptide reminiscent of prions. Since the content of pyroglutamylated
Aβ can vary up to 50% of total Aβ,[27,34,35] we studied pE-Aβ/Aβ samples
at 1:9 and 1:1 molar ratios in addition to pure Aβ and pE-Aβ
peptides. TEM images were acquired at 2, 4, 12, and 24 h of incubation,
as described in the Materials and Methods.
Most significant differences between Aβ1–42 and AβpE3-42 were detected at the early
stages of aggregation. At 2 h, the samples of AβpE3-42 were dominated by nonfibrillar aggregates of irregular shape and
average dimension of 30–100 nm, while the Aβ1–42 samples showed well-defined fibrils and a smaller number of small
aggregates (Figure 1a and b). The 1:9 and 1:1
molar combinations contained predominantly prefibrillar structures
(Figure 1c and d). At 4 h of incubation, the
fibrils were seen in all samples, with little morphological differences,
with small aggregates still present (Figure 1e–h). With progression of fibrillogenesis through 24 h, the
small aggregates were converted to fibrils which became more extended
and entangled (Figure 1i–p). While the
mature fibrils formed by the AβpE3-42 peptide
seem to be thicker, possibly bundled (cf. part n of Figure 1 with parts m, o, and p), consistent with earlier
observations,[24,28] the TEM data do not allow identification
of more distinct, definitive morphological differences between the
fibrils of the unmodified and pyroglutamylated peptides and their
combinations. Taking into account the clear differences between the
early stage assemblies of Aβ1–42 and AβpE3-42, these data suggest that the fibrillogenesis
of the two forms may follow different pathways, leading to fibrils
that are similar at the level of morphology. The images obtained in
negative control experiments showed clear grids, as expected (not
shown).
Figure 1
TEM images of Aβ1–42 (a, e, i, m), AβpE3-42 (b, f, j, n), AβpE3-42/Aβ1–42 = 1:9 (c, g, k, o), and AβpE3-42/Aβ1–42 = 1:1 (d, h, l,
p) incubated in aqueous buffer of 50 mM NaCl + 50 mM Na,K-phosphate
(pH 7.2) for 2 h (a–d), 4 h (e–h), 12 h (i–l),
and 24 h (m–p) at 37 °C with constant stirring. The horizontal
bar in each panel equals 100 nm.
TEM images of Aβ1–42 (a, e, i, m), AβpE3-42 (b, f, j, n), AβpE3-42/Aβ1–42 = 1:9 (c, g, k, o), and AβpE3-42/Aβ1–42 = 1:1 (d, h, l,
p) incubated in aqueous buffer of 50 mM NaCl + 50 mM Na,K-phosphate
(pH 7.2) for 2 h (a–d), 4 h (e–h), 12 h (i–l),
and 24 h (m–p) at 37 °C with constant stirring. The horizontal
bar in each panel equals 100 nm.Earlier TEM studies showed similar morphologies of AβpE3-42 and Aβ1–42 aggregates
at the initial stages of aggregation but more “curvilinear
and entangled” fibrils of Aβ1–42 at
1–2 days of fibrillogenesis.[38,39] In the equimolar
sample, the fibrils were less entangled, i.e. more like AβpE3-42 fibrils, suggesting that pE-Aβ might be
able to dictate its morphological (and probably structural) features
to the aggregates.It has been recognized that the fibrillar
morphology is determined
by the molecular structure of the peptides,[23,30,38,39] but CD studies
provided conflicting data on the relative secondary structural changes
in Aβ and pE-Aβ during fibrillogenesis (see above). To
monitor the structural transitions in the peptides during fibrillogenesis,
peptide samples dried from HFIP solution were used as a starting point,
before the onset of aggregation. CD spectra of Aβ1–42, AβpE3-42, and their combinations in dry
form shown in Figure 2a indicate mostly α-helical
structure with two minima around 222 and 208 nm.[40,41] The spectrum of AβpE3-42 has a significantly
reduced ratio of ellipticities θ208/θ222, indicative of a more flexible or disordered α-helix.[42] These results concur with solution NMR data
showing α-helical conformation for both Aβ1–42 and AβpE3–40 in organic solvents.[9,29] Upon addition of an aqueous buffer and incubation at 37 °C
with constant stirring, the peptides undergo significant structural
changes. Aβ1–42 promptly adopts and maintains
β-sheet structure, as evidenced by a deep minimum at 215–216
nm of spectra measured at 1 and 24 h of incubation (Figure 2b). The spectra of AβpE3-42, on the other hand, show a wide well between 208 and 222 nm, most
likely indicating a combination of α-helical and β-sheet
structures (Figure 2c). These data suggest
substantially different structures of Aβ1–42 and AβpE3-42, while the former readily adopts
β-sheets, the latter shows increased α-helical propensity.
The CD spectra of the 1:9 AβpE3-42/Aβ1–42 combination display β-sheet features, i.e.
a prominent minimum at 216 nm at 1 h and at 219 nm at 24 h of incubation
(Figure 2d). The higher intensity and the red
shift of the signal at 24 h may reflect gradual suspension of the
peptide into the aqueous medium and decreased solvent accessibility
upon aggregation.[40] It should be noted
that the spectra of Figure 2d are dominated
by the structural features of Aβ1–42 which
are present at a large molar excess (90%). At 1:1 molar ratio, the
1-h spectrum shows a minimum at 209 and a shoulder at 223 nm (Figure 2e), implying α-helix structure, possibly including
a β-sheet component, as in the case of pure AβpE3-42 (cf. blue spectra in Figure 2c and e). At
24 h, the spectrum has a β-sheet minimum at 216 nm and a shoulder
at 227 nm, likely generated by a turn structure. It is remarkable
that AβpE3-42 exerts a dominant structural
effect, especially at the early stages of fibrillogenesis. Thus, consistent
with the TEM data, CD results indicate that (a) Aβ1–42 and AβpE3-42 evidently follow distinct structural
pathways of fibrillogenesis and (b) AβpE3-42 is able to divert the overall path toward less β-sheet and
more α-helical intermediates.
Figure 2
CD spectra of dry and water-suspended
peptides. (a) Aβ1-42 (green), AβpE3-42 (turquoise),
AβpE3-42/Aβ1–42 =
1:9 (blue), and AβpE3-42/Aβ1–42 = 1:1 (red) were dissolved in HFIP, followed by 15 min of desiccation
in a 4 mm × 4 mm quartz cuvette and collection of the spectra.
(b–e) Aqueous buffer of 50 mM NaCl + 50 mM Na,K-phosphate (pH
7.2) was added to a 50 μM final concentration of Aβ1–42 (b), AβpE3-42 (c), AβpE3-42/Aβ1–42 = 1:9 (d), and
AβpE3-42/Aβ1–42 =
1:1 (e), and spectra were acquired after 1 h (blue) and 24 h (red)
of incubation at 37 °C with constant stirring.
CD spectra of dry and water-suspended
peptides. (a) Aβ1-42 (green), AβpE3-42 (turquoise),
AβpE3-42/Aβ1–42 =
1:9 (blue), and AβpE3-42/Aβ1–42 = 1:1 (red) were dissolved in HFIP, followed by 15 min of desiccation
in a 4 mm × 4 mm quartz cuvette and collection of the spectra.
(b–e) Aqueous buffer of 50 mM NaCl + 50 mM Na,K-phosphate (pH
7.2) was added to a 50 μM final concentration of Aβ1–42 (b), AβpE3-42 (c), AβpE3-42/Aβ1–42 = 1:9 (d), and
AβpE3-42/Aβ1–42 =
1:1 (e), and spectra were acquired after 1 h (blue) and 24 h (red)
of incubation at 37 °C with constant stirring.While TEM and CD data indicate distinct structural
differences
between Aβ1–42 and AβpE3-42 and suggest a dominant structural effect of pE-Aβ on Aβ,
neither of these methods has the capability of resolving the individual
structures of the two peptides in combination and the mutual structural
effects. Individual structures of two proteins combined in one sample
can be determined by FTIR spectroscopy if their amide I bands are
spectrally separated, which is achieved by 13C-labeling
of one of the proteins.[43−45] Despite its resolving power,
such “isotope-edited” FTIR spectroscopy has not been
used to characterize the concomitant structural transitions of Aβ
and pE-Aβ during fibrillogenesis.To detect the structural
changes accompanying formation of amyloid
fibrils, FTIR spectra were measured before and after exposure of the
peptides to an aqueous buffer. Both peptides were dissolved in HFIP
and dried on a CaF2 window by 15 min desiccation. AβpE3-42 adopts an intramolecular antiparallel β-sheet
structure (peak at 1634 cm–1 and shoulder around
1695 cm–1), as well as a significant fraction of
α-helix and turn structures (broad component(s) between 1685
and 1650 cm–1) (Figure 3a).[45−47]13C-Aβ1–42 forms an intermolecular
β-sheet (main peak at 1588 cm–1) plus turns
and an insignificant α-helix (component at 1617 cm–1) (Figure 3a). These data imply that 13C-Aβ1–42 readily forms a cross-β
structure even in the absence of an aqueous medium while AβpE3-42 forms intramolecular β-hairpins and an
α-helix. In aqueous (D2O) buffer, both peptides adopt
parallel intermolecular β-structure, as evidenced by the major
amide I peaks at 1628 cm–1 for AβpE3-42 and 1585 cm–1 for 13C-Aβ1–42 (Figure 3b). However, the
prominent component between 1680 and 1650 cm–1 in
the spectra of AβpE3-42 indicates that the
pyroglutamylated peptide retains significant fractions of α-helical
and turn structures. (The small peak in the spectra of 13C-A1–42 at 1673 cm–1 is likely
generated by trace amounts of trifluoroacetic acid usually present
in synthetic peptide samples.)
Figure 3
(a) FTIR spectra of AβpE3-42 (solid) and
uniformly 13C-labeled Aβ1–42 (dotted)
dried from a 200 μM HFIP solution on a CaF2 window.
(b) FTIR spectra of the two peptides, as indicated, in 10 mM Na,K-phosphate
in D2O, pD 7.2. Decreasing line darkness corresponds to
time of exposure of the peptides to the buffer for 10, 30, 50, 70,
90, and 120 min.
(a) FTIR spectra of AβpE3-42 (solid) and
uniformly 13C-labeled Aβ1–42 (dotted)
dried from a 200 μM HFIP solution on a CaF2 window.
(b) FTIR spectra of the two peptides, as indicated, in 10 mM Na,K-phosphate
in D2O, pD 7.2. Decreasing line darkness corresponds to
time of exposure of the peptides to the buffer for 10, 30, 50, 70,
90, and 120 min.The amide II spectral
region provides additional structural information
on proteins and peptides. Flexible secondary structures or open, solvent
accessible tertiary structures undergo faster amide hydrogen/deuterium
exchange resulting in reduction of the amide II band intensity around
1540 cm–1.[45−47] A considerable amide II band
is retained in the spectrum of 13C-Aβ1–42 after a 2 h exposure to D2O while that of AβpE3-42 is lost (Figure 3b), indicating
Aβ1–42 forms a rigid secondary structure and/or
a tight, solvent-inaccessible tertiary structure, characteristic of
a cross β-sheet structure,[10,11] while AβpE3-42 has a more open tertiary structure and/or more
flexible secondary structure.FTIR spectra of AβpE3-42 and 13C-Aβ1–42 combined at 1:9
(a) and 1:1 (b)
molar ratios, incubated in a D2O-based phosphate buffer
(pD 7.2) for 2 h, at a total peptide concentration of 100 μM.
Black and gray lines are the experimental spectra obtained on the
two peptides combined in one sample and the weighted sums of individual
spectra, respectively. The weighted sums were obtained as A = ∑fA, where f is the molar fraction and A is the absorbance spectrum of each
individual peptide measured separately.It has been shown earlier that isotope-edited FTIR can be
used
to probe the intermolecular interactions of peptides.[43,44] In the case of closely spaced 13C-labeled peptide units,
through H-bonding or through space 13C–13C vibrational coupling between adjacent strands results in a lower
frequency (∼1590–1594 cm–1) amide
I mode whereas 13C–12C coupling between
labeled and unlabeled units generates higher frequency (∼1600–1604
cm–1) components of enhanced intensity.[20,48,49] FTIR studies were conducted on
combined 13C-Aβ1–42 and unlabeled
AβpE3-42 to probe (a) the intermolecular interactions
and (b) mutual structural effects of the peptides. Since pE-Aβ
in AD brain can constitute up to 50% of total Aβ,[34,35] we studied AβpE3-42/13C-Aβ1–42 samples at 10% and 50% molar fractions of AβpE3-42. Data of Figure 4 indicate
that the β-sheet peak of 13C-Aβ1–42 at 1585 cm–1 up-shifts by 3 and 10 cm–1 in the presence of 10% and 50% pE-Aβ, respectively, while
the β-sheet peak of AβpE3-42 at 1626–1628
cm–1 up-shifts by 10 and 4 cm–1 in the presence of 90% and 50% 13C-Aβ1–42, respectively, indicating strong interactions and vibrational couplings
between the two peptides. Thus, AβpE3-42 and
Aβ1–42 form a mixed β-sheet structure
with tight intermolecular interactions.
Figure 4
FTIR spectra of AβpE3-42 and 13C-Aβ1–42 combined at 1:9
(a) and 1:1 (b)
molar ratios, incubated in a D2O-based phosphate buffer
(pD 7.2) for 2 h, at a total peptide concentration of 100 μM.
Black and gray lines are the experimental spectra obtained on the
two peptides combined in one sample and the weighted sums of individual
spectra, respectively. The weighted sums were obtained as A = ∑fA, where f is the molar fraction and A is the absorbance spectrum of each
individual peptide measured separately.
Next, we tested the
emerging hypothesis that the pyroglutamylated
peptide is able to modulate the structure of the unmodified Aβ
during amyloid fibril formation. To assess early structural events
in aggregation, combinations of HFIP solutions of AβpE3-42 and 13C-Aβ1–42 were dried on
a FTIR CaF2 window followed by collection of spectra while
the sample was allowed to absorb atmospheric humidity. Figure 5a shows the spectra of AβpE3-42 and 13C-Aβ1–42 combined at 1:9
molar ratio in a wide spectral range. The 1700–1500 cm–1 region corresponds to the amide I and amide II modes
and reflects the peptides’ secondary and dynamic structure
whereas the signal in the 3450–3150 cm–1 region
results from the amide A and H2O stretching modes.[45−47] Spectra shown in gray and black solid lines in Figure 5a and b were collected on a sample that was dried by desiccation
and exposed to the atmosphere for 10 and 20 min, respectively. The
peptides absorb atmospheric humidity, which results in an increase
in the H2O stretching band around 3270 cm–1. Nominal hydration causes conformational transitions in both peptides
and corresponding spectral changes in the amide I region, shown in
Figure 5b. At a 1:9 AβpE3-42/13C-Aβ1–42 molar ratio, the amide
I band is dominated by the spectral features of the latter peptide,
i.e. α-helical and β-sheet components at 1617 and 1592
cm–1, respectively (Figure 5b). The broad band around 1655 cm–1 evidently results
from the overlapped α-helical mode of AβpE3-42 and the turn structures of 13C-Aβ1–42. As the sample absorbs atmospheric moisture, 13C-Aβ1–42 undergoes α-to-β transition (intensity
transfer from 1617 to 1592 cm–1, cf. gray and black
solid lines in Figure 5b). However, a more
humid 1:9 mixture (black solid line) contains less β-sheet and
more α-helix than expected without interaction between the two
peptides (the weighted sum of individual spectra shown in a dotted
line). These and above data suggest that pE-Aβ slows down cross
β-sheet formation in Aβ by direct intermolecular interactions.
Figure 5
FTIR spectra
of AβpE3-42 and uniformly 13C-labeled
Aβ1–42 at 1:9 molar ratio
(a and b) and 1:1 molar ratio (c). Gray and black solid lines are
experimental spectra of a sample prepared in HFIP, followed by solvent
removal by desiccation and exposure to atmosphere for 10 and 20 min,
respectively. The dotted spectrum is the weighted sum of the spectra
of each peptide measured individually, exposed to the atmosphere for
15 min. Construction of the weighted sum spectra is described under
Figure 4. Panel b is a zoom-in into the amide
I/II region of spectra shown in panel a.
FTIR spectra
of AβpE3-42 and uniformly 13C-labeled
Aβ1–42 at 1:9 molar ratio
(a and b) and 1:1 molar ratio (c). Gray and black solid lines are
experimental spectra of a sample prepared in HFIP, followed by solvent
removal by desiccation and exposure to atmosphere for 10 and 20 min,
respectively. The dotted spectrum is the weighted sum of the spectra
of each peptide measured individually, exposed to the atmosphere for
15 min. Construction of the weighted sum spectra is described under
Figure 4. Panel b is a zoom-in into the amide
I/II region of spectra shown in panel a.Moreover, at 1:1 molar combination, pE-Aβ reverses
the cross-β
structure and hence fibrillization of Aβ. As shown in Figure 5c, in the presence of 50% pE-Aβ, the intermolecular
β-sheet peak of 13C-Aβ1–42 shifts from 1588 to 1595 cm–1 (cf. dotted and
gray spectra), indicating strong interaction between the two peptides.
(In the presence of only 10% AβpE-42, a smaller
shift from 1588 to 1592 cm–1 is observed, Figure 5b.) In the presence of an equimolar amount of AβpE3-42, there is no α-helix to β-sheet conversion
of 13C-Aβ1–42 over time, as seen
by the similar signal intensity at 1617 cm–1 in
gray and black solid spectra in Figure 5c.
Most importantly, AβpE3-42 causes a strong
reduction of the intermolecular β-sheet signal of 13C-Aβ1–42 at 1595 cm–1 during
longer coincubation (cf. gray and black solid spectra in Figure 5c) paralleled with increased intensity around 1658
cm–1. The spectra of the combination (gray and black
solid lines in Figure 5c) indicate an increase
in α-helical structure (signals at 1658 and 1617 cm–1) and a decrease in β-sheet structure (signals at 1634 and
1585–1588 cm–1) in both peptides as compared
to the weighted sum of individual spectra (dotted line in Figure 5c). Although the component at 1658 cm–1 might partially result from turn structures in addition to the α-helix
in AβpE3-42, these data identify prominent
mutual conformational effects of the two peptides; pE-Aβ at
10% delays cross β-sheet formation and hence fibrillization
and at 50% reverses the cross β-sheet structure formation of
Aβ.
Discussion
Our data identify significant
differences between AβpE3-42 and Aβ1–42 at the levels
of morphology as well as secondary and tertiary structures. At the
initial stages of fibrillogenesis, the pyroglutamylated AβpE3-42 peptide forms more prefibrillar aggregates, apparently
due to its increased hydrophobicity, and it undergoes fibril elongation
slower than the unmodified Aβ1–42 peptide
(Figure 1a,b), in agreement with earlier data.[31] Retardation of fibrillization appears to be
imparted to Aβ1–42 even at low molar contents
of AβpE3-42 (Figure 1c). CD data indicate augmented α-helical and diminished β-sheet
propensity of AβpE3-42, which is transmitted
to the mixed assemblies (Figure 2). FTIR indicates
that the unmodified peptide readily forms a tightly packed intermolecular
β-sheet, while pE-Aβ forms a less compact β-structure
and contains more α-helix and turn structures than Aβ
(Figure 3). Furthermore, the pyroglutamylated
peptide not only exhibits a significantly lower tendency to form a
β-sheet structure but also inhibits cross β-sheet formation
in the unmodified peptide through direct interactions (Figures 4 and 5). These structural
transitions occur rapidly upon hydration, but they can be captured
when the peptides undergo nominal hydration by exposure to atmospheric
humidity. These conditions are both technically beneficial and meaningful
because the fibrils formed by Aβ1–40 were
shown to contain an extremely low fraction of water, i.e., an average
of 1.2 water molecules per β-strand.[50] Significant retention of the amide II band in the spectrum of Aβ1–42 in a D2O-based buffer (Figure 3b) is in line with this finding. Furthermore, the
rapid loss of the amide II band of AβpE3-42 upon exposure to D2O indicates a more flexible secondary
and/or a more open tertiary structure of the pyroglutamylated peptide.If pE-Aβ eventually forms fibrils that contain β-sheet
structure, even though different from the fibrils formed by unmodified
Aβ, why do the intermediate structural steps matter? The answer
is that the oligomeric, prefibrillar assemblies of Aβ that adopt
still poorly characterized “pathological conformation“
are the most toxic species.[51] For example,
the secreted pool of Aβ oligomers exerts its toxic effect partly
by binding to a set of receptors, including the insulin receptor that
recognizes an α-helical ligand.[51] Intracellular oligomers bind to the mitochondrial or endoplasmic
reticulum proteins and cause cell damage through oxidative stress
or calcium dysregulation before they are secreted.[52,53] Since the cytotoxic effect is exerted before formation of the extracellular
deposits, chracterizaton of the intermediate “pathological
conformations“ is crucial.The structural impact of pE-Aβ
on the unmodified peptide
even at low molar content (10%) is indicative of a prion-like effect.
The pE-Aβ peptide tightly interacts with Aβ, as indicated
by efficient 12C–13C vibrational coupling
(Figures 4 and 5), and
thereby transmits the specific structural features to the unmodified
peptide. Data of Figures 2–5 strongly imply that this specific structure is
rich in α-helix as opposed to β-sheet. This effect takes
place even at 10% pE-Aβ, when pE-Aβ molecules cannot simultaneously
interact with a large excess of unmodified Aβ. We therefore
propose that once the structural transition occurs in the unmodified
Aβ molecule by its interaction with pE-Aβ, it acquires
the capability to further transmit the altered structure to other
Aβ peptides by direct interaction. This prion-like conformational
effect of pE-Aβ may eventually shift the overall path of peptideaggregation toward formation of hypertoxic, lower molecular weight
aggregates of partial α-helical structure and thus suppress
formation of less toxic cross β-sheet fibrils.
Authors: Thorsten Lührs; Christiane Ritter; Marc Adrian; Dominique Riek-Loher; Bernd Bohrmann; Heinz Döbeli; David Schubert; Roland Riek Journal: Proc Natl Acad Sci U S A Date: 2005-11-17 Impact factor: 11.205
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